A non-Hermitian quasicrystal model exhibits coexistence of a topological Anderson insulator phase and a multifractal critical phase, with exact analytical boundaries for both topological and localization transitions.
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In a non-Hermitian Kitaev chain with staggered pairing imbalance, tuning parameters induces an enlarged topological phase supporting Majorana zero modes and their coexistence with finite-energy edge modes.
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Coexistence of topological Anderson insulator and multifractal critical phase in a non-Hermitian quasicrystal
A non-Hermitian quasicrystal model exhibits coexistence of a topological Anderson insulator phase and a multifractal critical phase, with exact analytical boundaries for both topological and localization transitions.
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Topological superconducting phase in a non-Hermitian Kitaev chain with staggered pairing imbalance
In a non-Hermitian Kitaev chain with staggered pairing imbalance, tuning parameters induces an enlarged topological phase supporting Majorana zero modes and their coexistence with finite-energy edge modes.